where, the coupling constant \(g=0.59 \pm 0.07 \pm 0.01\)  is extracted from the width of \(D^{*}\)  [1]}, [2]}, \(g_{1}= 0.75, 0.94, 1.95\)  [3]}, [4]}. Also, it is the mass of pion \(m_{\pi }=135 MeV\)  and pion decay constant \(f_{\pi }=132 MeV\)  [5]}. The amount of phenomenological cutoff parameter is considered \(\Lambda =0.8 GeV-2.5 GeV\)  [5]}, [7]}. Finally, the \(Y(\Lambda , m_{\pi }, r)\)  is [5]}:
\(Y(\Lambda , m_{\pi }, r)= \frac{1}{4 \pi r}\ (e^{-m_{\pi }r} - e^{-\Lambda r})-\frac{\Lambda ^{2}-m_{\pi }^{2}}{8 \pi \Lambda }\ e^{-\Lambda r}.\) 
